Optical frequency acquisition apparatus for optical coherent communication system

Abstract: An automatic frequency control system, for an optical coherent communication system, in which the frequency of local oscillation light 5 from coherent light communication receiver 100 are swept to pull the intermediate frequency at a stable AFC point. The AFC is caused to operate with an intermediate frequency in the AFC operation range, and interrupted. Subsequently while sweeping the frequency of local oscillation light 5 in a certain direction in a predetermined range, the output voltage of frequency discriminator 9 is monitored. Once the change of the output voltage of frequency discriminator 9 due to the sweep exceeds the predetermined threshold value, the AFC resumes for the pulling to a stable point.

Description: The present invention relates to an optical coherent communication system, and particularly to a technique for controlling intermediate frequency in an optical heterodyne detection system. Optical heterodyne communication (Optical coherent communication) system is advantageous in that a long distance, high capacity transmission is possible because reception sensitivity is much higher compared with a direct detection communication system and because it is suitable for a frequency division multiplexed system. In an heterodyne detection system, a photo detector receives a composite signal of an input optical signal transmitted from a transmitter and a local oscillation light from a local oscillation light source included in an optical receiver thereof. As a result, a beat corresponding to a frequency difference therebetween appears at an output of the photo detector as an electric intermediate frequency (IF) signal. By demodulating this IF signal, a base band signal is obtained. When the relative frequency difference between the signal light and the local oscillation light is not maintained constant, fluctuation of the IF occurs, resulting in an error in a demodulated signal. Therefore in the optical heterodyne detection system, the IF frequency has to be stabilized by controlling the local oscillation light frequency. For this IF stabilization, the automatic frequency control (AFC) technique is used. In conventional optical heterodyne receivers, for realization of AFC, an IF signal is put into a frequency discriminator with a characteristic of zero-crossing at a desired IF value and the output signal from it is fed back as an injection current to a semiconductor laser working as a local oscillation light source. By the way, in the optical heterodyne receiver, with the same IF, the frequency of the local oscillation light can be higher in some cases or lower in other cases than the frequency of the signal light. Correspondingly there are real and image bands. The characteristics of IF frequency vs. frequency discriminator output voltage utilized for AFC in the real and image bands are opposite to each other, and stable AFC points appears in both bands. A demodulated signal in the image band has poor quality as well known in the art. A method for pull-in to a desired stable AFC point in the real band is disclosed in USP No. 5,046,140. This method involves sweeping the frequency of the local oscillation light while making a slight frequency modulation of local oscillation light, detecting the differential rate of the output signal voltage of a frequency discriminator using lock-in amplifier, or the like, and decide whether real or image band based on the result of positive or negative of the differential rate. This method however takes a long pull-in time since it needs to sweep the frequency of the local oscillation light over the whole band including both real and image bands. This long pull-in time, particularly when receiving a frequency-division multiplexed signal with need for channel switch, places a severe restriction on operation of the system. EP-A-0 396 370 discloses a random-access digitally-tuned coherent optical receiver with a local oscillator, an IF-band signal producing means and a frequency discriminator. It is the principal object of the present invention to provide an optical frequency acquisition apparatus for optical coherent communication system permitting to quickly make distinction between real and image bands. This object is achieved with the features of the claims. Fig. 1 is a block diagram of an embodiment of the present invention; Fig. 2 shows an example of the input-IF frequency vs. output voltage characteristic of the frequency discriminator; Fig. 3 shows the frequency difference between a signal light frequency and a local oscillation light frequency vs. output voltage characteristic of the frequency discriminator; Fig. 4 is a flow chart for illustrating the operation of controller 11 in the first embodiment of the present invention; Fig. 5 shows the input IF frequency vs. output voltage characteristic of the frequency discriminator in the second embodiment of the present invention; and Fig. 6 is a flow chart for illustrating the operation of controller 11 in the second embodiment of the present invention. The invention will be set forth with reference to the accompanying drawing hereinafter. Fig. 1 is a block diagram of an illustrative example of the structure of a 600 Mb/s FSK (frequency shift keying) optical heterodyne receiver. A signal light 2 transmitted through an optical fiber 1 is combined with a local oscillation light 5 emitted from a laser 4 by a light coupler 3, and is detected by photo-detectors 6. The operational temperature of local oscillation laser 4 is controlled at 25°C constantly by a temperature stabilizing mechanism (not shown). The photo-detectors 6 output an IF electrical signal which is amplified in an IF amplifier 7 and is put into a demodulator (DEM) 8 and a frequency discriminator (DISC) 9. Frequency discriminator 9 shows a discriminative characteristic with the right-falling zero-crossing point at 2.5 GHz as shown in Fig. 2. In Fig. 3 there are two stable AFC operation points "A" and "B" each in the real and image bands, respectively. A demodulator 8 extracts the 600 Mb/s baseband signal from the IF signal by the dual filter detection and is adjusted to normally operate at point "A" in Fig. 3. Frequency discriminator 9 outputs a voltage signal through an analog-digital converter (A/D) 10 to a controller (CONT) 11 which controls the injection current to local oscillation laser 4 through a digital-analog converter (D/A) 12 and a current driver (DRV) 13 which contributes to setting the frequency of local oscillation light 5. Additionally referring to Fig. 4, the operation of controller 11 will be set forth. Controller 11 consists, for example, of a microcomputer, and operates as shown in the flow chart of Fig. 4. Once receiver 100 is turned on, or switch to any channel to be used is caused, controller 11 supplies the corresponding initial current value I o (λ) stored therein to the channel to current driver 13 which feeds an injection current to the local oscillation laser, and thereby causes receiver 100 to make the AFC operation (step S1). As well-known, this AFC operation will be performed as follows. Now assume that as the local oscillation laser oscillator is used such that has a characteristic of having higher frequency (or the shorter wavelength) with increasing injection current. During this AFC operation in step S1, controller 11, when the output-voltage dc component of frequency discriminator 9 of which the characteristic is plotted in Fig. 3 is positive, reduces the injection current value to lower the oscillation frequency (f Lo ) of local oscillation laser 4, and when negative, increases the injection current to increase the oscillation frequency (f Lo ). When the output voltage of frequency discriminator 9 becomes about zero under the above-mentioned AFC, controller 11 stores the injection current value i o fed to the local oscillation laser at this time, and receiver 100 stays at stable AFC operation point either "A" or "B" in Fig. 3. In step S2, controller 11 adds a predetermined current value Δi, which is enough to increase the oscillation frequency of the local oscillation laser by the predetermined value, to current value i o , the resultant injection current i = i o + Δi being fed to local oscillation laser 4. In the next step S3, controller 11 measures the increased output voltage ΔV of the frequency discriminator due to the added injection current value Δi. In step S4, controller 11 checks whether or not the output voltage change | ΔV | of the frequency discriminator is larger than the predetermined voltage value TH. If | ΔV | > TH, the operation of the controller 11 transfers to step S5, and if not so, to step S6. Decision of | ΔV | > TH in step S4 means that under the AFC operation in step S1 receiver 100 stays at stable AFC point "A" shown in Fig. 3 while decision of ΔV ≦ TH, if the same except this, means it stays at another stable AFC point 3. In the example of Fig. 3, TH = 1.0 V, and the oscillation frequency increase of the local oscillation laser due to injection current increase Δi is set to 1.0 GHz. In step S5, injection current "i" to local oscillation laser 4 is returned to i o . The operation of controller 11 transfers to the next step S7, and the AFC operation restarts and rapidly converges because it starts at the near stable point A. When pulled, in step S1, into the real band by the operations of steps S1 through S6 and S7, receiver 100 continues to operate in the real band. In step S6, controller 11 adds a current value (-ΔI) enough to shift the local oscillation frequency f Lo from stable point "B" to stable point "A" to i o , and causes current driver 13 to feed the resultant injection current (i o - ΔI) to the local oscillation laser 4, resulting in the shift of the IF frequency to the near stable point A. The AFC operation resumes in step S7. According to the first embodiment described above, the time taking from the turn-on to when the AFC operation has converged in step S7 was measured of 20 runs to get an average value of 9.2 msec while according to the process described in USP No. 5,046,140, it took 122 msec for the pull-in at the stable point to the real band. The first embodiment was described by the example of setting AFC operation center at the zero-crossing point "A" in the right-rising part of the characteristic of (f Lo - f in ) vs. output voltage. According to the present invention, also a frequency discriminator which has such characteristic of (f Lo - f in ) vs. output voltage as shown in Fig. 5 can be used. An alternative (the second) embodiment in which the present invention is applied to a frequency discriminator having the characteristic of Fig. 5 will be described below with reference to Figs. 5 and 6. The example of Fig. 5 will be set forth assuming to set the AFC operation center to point "A'". In this case there are AFC operation points "B'" and "C'" in the image band. In this embodiment of Fig. 5, because of setting at the zero-crossing point in the right-falling part of the (f Lo - f in ) vs. output voltage characteristic, the AFC operation of controller 11 is made as follows: when the output of the frequency discriminator is positive, the injection current increases and thereby the oscillation frequency of the local oscillation laser increases and when negative, vice versa. Referring to Fig. 6, the operation of controller 11 in the second embodiment of the present invention will be described. First, in step S21, controller 11 causes current driver 13 to feed initial current value I o (λ) stored therein corresponding to a desired channel to the local oscillation laser, and in response to this, receiver 100 performs the AFC operation. Once the output of the frequency discriminator reaches approximately zero V, controller 11 stores the injection current value i o to the local oscillation laser 4. In the next step S22, controller 11 adds a certain current value Δi enough to increase the oscillation frequency of the local oscillation laser 4 by the predetermined value to current value i o , and causes current driver 13 to feed the added injection current i = i o + Δi to local oscillation laser 4. Then controller 11 measures, and stores, the output voltage change ΔV 1 of the frequency discriminator 9 due to the injection-current increase Δi. In step S23, the injection current value to local oscillation laser is caused to change from i o to i o - Δi, and the thereby-change ΔV 2 of output voltage of the frequency discriminator due to the injection current decrease (-Δi) is measured and stored. In step S24, | ΔV 1 | is compared with the predetermined voltage TH. If | ΔV 1 | > TH, the operation of controller 11 transfers to step S25, and if | ΔV 1 | ≦ TH, the operation to step S28. By the way in the example of Fig. 5 the increase of local oscillation frequency associated with injection current-increase Δi is set to 0.5 GHz, and TH to 1.0 V. As apparent from Fig. 5, even if oscillation frequency f Lo is increased by 0.5 GHz, | ΔV 1 | can not be smaller than TH (= 1.0 V) except the case receiver 100 stays at stable point C'. Shift of the AFC operation center from this stable point C' to stable point A' is allowed by 4.0 GHz decrease of f Lo . In step S28 therefore controller 11 adds a current value (-ΔI 2 ) enough to reduce the oscillation frequency by 4 GHz to current value i o , the resultant current value (i o - ΔI 2 ) being fed as the AFC initial-value current to the local oscillation laser, and in the next step S29 the AFC operation restarts. In step S25, controller 11 compares | ΔV 2 | with TH. If | ΔV 2 | > TH, the operation of it transfers to step S26, and if not so, to step S27. In step S26, the injection current value is set again to i o and fed as the AFC initial current to local oscillation laser 4, and then controller 11 accomplishes the AFC operation in step S29. The transfer the operation of controller 11 to step S26 means | ΔV 1 | > TH and | ΔV 2 | > TH. As appeared from Fig. 5, these two conditions can not be met except the case receiver 100 stays at stable point A' in step S21. In step S26 therefore the injection current to the local oscillation laser is returned to i o . Transfer of the operation of controller 11 to step S27 is made in the case receiver 100 stays at stable point B' in step S21. In this case, 2 GHz-decrease in local oscillation frequency f Lo results in the shift of the AFC operation center to point A'. For this reason, in step S27, controller 11 adds a current value ( - ΔI 1 ) enough to reduce the local oscillation frequency f Lo by 2 GHz to current value i o , the resultant current value (i o - ΔI 1 ) being fed as the AFC operation initial-value current to the local oscillation laser. In this way, in the second embodiment the operation of the receiver stays at a desired stable AFC operation point A'. As described above, the present invention permits, even if frequency discriminator used for the AFC has a plurality of stable points each in the real or image bands, respectively, the rapid, exact pull-in of the intermediate frequency into a stable point in the real band without needing sweep of the local oscillation frequency over the whole including the real or image bands as in the conventional way.

Claims: An optical frequency acquisition apparatus for optical coherent communication system, each of image and real bands of said apparatus having one stable AFC operation point, comprising: a local optical oscillator (4) responsive to an injection current and adapted for producing a local oscillation light (5); IF-band signal producing means (3,6,7) responsive to an optical input signal (2) and said local oscillation light (5) and adapted for producing an IF band signal; and a frequency discriminator (9) for discriminating said frequency of said IF signal; characterized by : a controller (11) for controlling what amount of injection current is produced based on a frequency discriminator output, said controller starting said AFC operation feeding said injection current dependent on said dc component of said frequency discriminator output to said local optical oscillator after feeding an initial injection current, and operating in the following three steps of (a), (b) and (c): (a) the first step for feeding a predetermined current value for each channel as said initial current value to said local optical oscillator (4) to perform said AFC operation, and storing said injection current value io at the time when said frequency discriminator output reaches almost zero; (b) the second step for changing said injection current value to (i o + Δi), where Δi is a constant current value, and measuring the dc component ΔV of said frequency discriminator output; and (c) the third step for restarting said AFC operation using i o as said initial injection current if the absolute value of said ΔV exceeds a predetermined value TH, and otherwise using (i o + ΔI) wherein ΔI is an injection current change needed to shift the operation of said apparatus from said stable AFC operation point in said image band to that in said real band. An apparatus according to claim 1, wherein said real band having one AFC operation point and said image band having first and second stable AFC operation points, and said controller operating in the following three steps of (a), (b) and (c); (a) the first step for feeding a predetermined current value for each channel as said initial current value to said local optical oscillator (4) to perform said AFC operation, and storing said injection current value i o at said time when said frequency discriminator output reaches almost zero; (b) the second step for changing said injection current value to (i o + Δi) and (i o - Δi), respectively, and measuring dc components ΔV 1 and ΔV 2 , of said frequency discriminator outputs, respectively; and (c) the third step for restarting said AFC operation using i o as said initial injection current if the respective absolute values of said ΔV 1 and ΔV 2 both exceed a predetermined value TH, using (i o + ΔI 1 ) if | ΔV 1 | > TH and | ΔV 2 | < TH, and using (i o + ΔI 2 ) if | ΔV 1 | < TH and | ΔV 2 | < TH, wherein, ΔI 1 is an injection current change needed to shift the operation of said apparatus from said first stable AFC operation point in said image band to that in said real band and ΔI 2 is an injection current change needed to shift the operation of said apparatus from said second stable AFC point in said image band to that in said real band.

Inventors: SUEMURA YOSHIHIKO, SUEMURA, YOSHIHIKO, SUEMURA, YOSHIHIKO, C/O NEC CORPORATION
Applicants: NIPPON ELECTRIC CO, NEC CORPORATION
Application year: 1994
Main classification: H04B10
IPC codes: H04B10